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A First Course in Linear Algebra, 2017a

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Chapter 1<br />

Systems of Equations<br />

1.1 Systems of Equations, Geometry<br />

Outcomes<br />

A. Relate the types of solution sets of a system of two (three) variables to the <strong>in</strong>tersections of<br />

l<strong>in</strong>es <strong>in</strong> a plane (the <strong>in</strong>tersection of planes <strong>in</strong> three space)<br />

As you may remember, l<strong>in</strong>ear equations like 2x +3y = 6 can be graphed as straight l<strong>in</strong>es <strong>in</strong> the coord<strong>in</strong>ate<br />

plane. We say that this equation is <strong>in</strong> two variables, <strong>in</strong> this case x and y. Suppose you have two such<br />

equations, each of which can be graphed as a straight l<strong>in</strong>e, and consider the result<strong>in</strong>g graph of two l<strong>in</strong>es.<br />

What would it mean if there exists a po<strong>in</strong>t of <strong>in</strong>tersection between the two l<strong>in</strong>es? This po<strong>in</strong>t, which lies on<br />

both graphs, gives x and y values for which both equations are true. In other words, this po<strong>in</strong>t gives the<br />

ordered pair (x,y) that satisfy both equations. If the po<strong>in</strong>t (x,y) is a po<strong>in</strong>t of <strong>in</strong>tersection, we say that (x,y)<br />

is a solution to the two equations. In l<strong>in</strong>ear algebra, we often are concerned with f<strong>in</strong>d<strong>in</strong>g the solution(s)<br />

to a system of equations, if such solutions exist. <strong>First</strong>, we consider graphical representations of solutions<br />

and later we will consider the algebraic methods for f<strong>in</strong>d<strong>in</strong>g solutions.<br />

When look<strong>in</strong>g for the <strong>in</strong>tersection of two l<strong>in</strong>es <strong>in</strong> a graph, several situations may arise. The follow<strong>in</strong>g<br />

picture demonstrates the possible situations when consider<strong>in</strong>g two equations (two l<strong>in</strong>es <strong>in</strong> the graph)<br />

<strong>in</strong>volv<strong>in</strong>g two variables.<br />

y<br />

y<br />

y<br />

x<br />

One Solution<br />

x<br />

No Solutions<br />

x<br />

Inf<strong>in</strong>itely Many Solutions<br />

In the first diagram, there is a unique po<strong>in</strong>t of <strong>in</strong>tersection, which means that there is only one (unique)<br />

solution to the two equations. In the second, there are no po<strong>in</strong>ts of <strong>in</strong>tersection and no solution. When no<br />

solution exists, this means that the two l<strong>in</strong>es are parallel and they never <strong>in</strong>tersect. The third situation which<br />

can occur, as demonstrated <strong>in</strong> diagram three, is that the two l<strong>in</strong>es are really the same l<strong>in</strong>e. For example,<br />

x + y = 1and2x + 2y = 2 are equations which when graphed yield the same l<strong>in</strong>e. In this case there are<br />

<strong>in</strong>f<strong>in</strong>itely many po<strong>in</strong>ts which are solutions of these two equations, as every ordered pair which is on the<br />

graph of the l<strong>in</strong>e satisfies both equations. When consider<strong>in</strong>g l<strong>in</strong>ear systems of equations, there are always<br />

three types of solutions possible; exactly one (unique) solution, <strong>in</strong>f<strong>in</strong>itely many solutions, or no solution.<br />

3

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